How to Evaluate Multivariable Limits
Try directly substituting first., Try substituting to make the limit single-variable when the substitution is obvious., If you suspect that the limit does not exist (DNE), show this by approaching from two different directions., Convert to polar...
Step-by-Step Guide
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Step 1: Try directly substituting first.
Sometimes, a limit is trivial to calculate
- similar to single-variable calculus, plugging in the values may immediately net you the answer.
This is usually the case when the limit does not approach the origin.
An example follows. lim(x,y)→(4,5)(x2y3−5xy2)=(4)2(5)3−5(4)(5)2=1500{\displaystyle {\begin{aligned}\lim _{(x,y)\to (4,5)}(x^{2}y^{3}-5xy^{2})&=(4)^{2}(5)^{3}-5(4)(5)^{2}\\&=1500\end{aligned}}} Another reason why substituting works here is that the function above is polynomial, and therefore is well-behaved across the reals for all x{\displaystyle x} and y.{\displaystyle y.} -
Step 2: Try substituting to make the limit single-variable when the substitution is obvious.
Evaluate lim(x,y)→(0,0)ln(1−5x2y2)12x2y2.{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {\ln(1-5x^{2}y^{2})}{12x^{2}y^{2}}}.} Substitute t=x2y2.{\displaystyle t=x^{2}y^{2}.} limt→0ln(1−5t)12t{\displaystyle \lim _{t\to 0}{\frac {\ln(1-5t)}{12t}}} Use L'Hôpital's rule, as currently we get a 00{\displaystyle {\frac {0}{0}}} if we evaluate too soon. limt→0ln(1−5t)12t=limt→011−5t(−5)12=−512.{\displaystyle {\begin{aligned}\lim _{t\to 0}{\frac {\ln(1-5t)}{12t}}&=\lim _{t\to 0}{\frac {{\frac {1}{1-5t}}(-5)}{12}}\\&={\frac {-5}{12}}.\end{aligned}}} , As long as the limit either DNE or is different from these two directions, you are finished and the limit of the overall function DNE.
Evaluate lim(x,y)→(0,0)x2−y2x2+y2.{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {x^{2}-y^{2}}{x^{2}+y^{2}}}.} Approach from both sides vertically and horizontally.
Set x=0{\displaystyle x=0} and y=0.{\displaystyle y=0.} lim(0,y)→(0,0)x2−y2x2+y2=lim(0,y)→(0,0)(0)2−y2(0)2+y2=−1.{\displaystyle \lim _{(0,y)\to (0,0)}{\frac {x^{2}-y^{2}}{x^{2}+y^{2}}}=\lim _{(0,y)\to (0,0)}{\frac {(0)^{2}-y^{2}}{(0)^{2}+y^{2}}}=-1.} lim(x,0)→(0,0)x2−y2x2+y2=lim(x,0)→(0,0)x2−(0)2x2+(0)2=1.{\displaystyle \lim _{(x,0)\to (0,0)}{\frac {x^{2}-y^{2}}{x^{2}+y^{2}}}=\lim _{(x,0)\to (0,0)}{\frac {x^{2}-(0)^{2}}{x^{2}+(0)^{2}}}=1.} Since the two limits are different, the limit DNE. , Multivariable limits are often easier when done in polar coordinates.
In this case, x=rcosθ{\displaystyle x=r\cos \theta } and y=rsinθ.{\displaystyle y=r\sin \theta .} Let’s see how this works. , lim(x,y)→(0,0)xy2x2+y2{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {xy^{2}}{x^{2}+y^{2}}}} , limr→0r3cosθsin2θr2=limr→0(rcosθsin2θ){\displaystyle \lim _{r\to 0}{\frac {r^{3}\cos \theta \sin ^{2}\theta }{r^{2}}}=\lim _{r\to 0}(r\cos \theta \sin ^{2}\theta )} , Although the limit is taken as r→0,{\displaystyle r\to 0,} the limit depends on θ{\displaystyle \theta } as well.
One might then naively conclude that the limit DNE.
However, the limit does depend on r,{\displaystyle r,} so the limit may or may not exist.
Since |sinθ|≤1{\displaystyle |\sin \theta |\leq 1} and |cosθ|≤1,|cosθsin2θ|≤1{\displaystyle |\cos \theta |\leq 1,|\cos \theta \sin ^{2}\theta |\leq 1} as well.
Then |rcosθsin2θ|≤r.{\displaystyle |r\cos \theta \sin ^{2}\theta |\leq r.} , Since limr→0(−r)=limr→0(r)=0,{\displaystyle \lim _{r\to 0}(-r)=\lim _{r\to 0}(r)=0,} by the Squeeze Theorem, limr→0(rcosθsin2θ)=0.{\displaystyle \lim _{r\to 0}(r\cos \theta \sin ^{2}\theta )=0.} Because of the r{\displaystyle r} dependency and the use of the Squeeze Theorem, the quantity in the above limit is said to be bounded.
In other words, as r→0,{\displaystyle r\to 0,} the range of values of rcosθsin2θ{\displaystyle r\cos \theta \sin ^{2}\theta } shrinks to 0 as well, even though θ{\displaystyle \theta } is arbitrary. , lim(x,y)→(0,0)xyx2+y2{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {xy}{x^{2}+y^{2}}}} This example is only slightly different from the one in Example
1. , limr→0r2cosθsin2θr2=limr→0(cosθsin2θ){\displaystyle \lim _{r\to 0}{\frac {r^{2}\cos \theta \sin ^{2}\theta }{r^{2}}}=\lim _{r\to 0}(\cos \theta \sin ^{2}\theta )} However, the quantity cosθsin2θ{\displaystyle \cos \theta \sin ^{2}\theta } can take on an arbitrary value after the limit is evaluated, and is said to be unbounded.
Therefore, the limit DNE.
This scenario is describing a limit being approached from arbitrary directions and getting different values. -
Step 3: If you suspect that the limit does not exist (DNE)
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Step 4: show this by approaching from two different directions.
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Step 5: Convert to polar form.
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Step 6: Evaluate the limit.
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Step 7: Convert to polar.
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Step 8: Use the Squeeze Theorem.
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Step 9: Take the limit of all three expressions.
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Step 10: Evaluate the limit.
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Step 11: Convert to polar.
Detailed Guide
Sometimes, a limit is trivial to calculate
- similar to single-variable calculus, plugging in the values may immediately net you the answer.
This is usually the case when the limit does not approach the origin.
An example follows. lim(x,y)→(4,5)(x2y3−5xy2)=(4)2(5)3−5(4)(5)2=1500{\displaystyle {\begin{aligned}\lim _{(x,y)\to (4,5)}(x^{2}y^{3}-5xy^{2})&=(4)^{2}(5)^{3}-5(4)(5)^{2}\\&=1500\end{aligned}}} Another reason why substituting works here is that the function above is polynomial, and therefore is well-behaved across the reals for all x{\displaystyle x} and y.{\displaystyle y.}
Evaluate lim(x,y)→(0,0)ln(1−5x2y2)12x2y2.{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {\ln(1-5x^{2}y^{2})}{12x^{2}y^{2}}}.} Substitute t=x2y2.{\displaystyle t=x^{2}y^{2}.} limt→0ln(1−5t)12t{\displaystyle \lim _{t\to 0}{\frac {\ln(1-5t)}{12t}}} Use L'Hôpital's rule, as currently we get a 00{\displaystyle {\frac {0}{0}}} if we evaluate too soon. limt→0ln(1−5t)12t=limt→011−5t(−5)12=−512.{\displaystyle {\begin{aligned}\lim _{t\to 0}{\frac {\ln(1-5t)}{12t}}&=\lim _{t\to 0}{\frac {{\frac {1}{1-5t}}(-5)}{12}}\\&={\frac {-5}{12}}.\end{aligned}}} , As long as the limit either DNE or is different from these two directions, you are finished and the limit of the overall function DNE.
Evaluate lim(x,y)→(0,0)x2−y2x2+y2.{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {x^{2}-y^{2}}{x^{2}+y^{2}}}.} Approach from both sides vertically and horizontally.
Set x=0{\displaystyle x=0} and y=0.{\displaystyle y=0.} lim(0,y)→(0,0)x2−y2x2+y2=lim(0,y)→(0,0)(0)2−y2(0)2+y2=−1.{\displaystyle \lim _{(0,y)\to (0,0)}{\frac {x^{2}-y^{2}}{x^{2}+y^{2}}}=\lim _{(0,y)\to (0,0)}{\frac {(0)^{2}-y^{2}}{(0)^{2}+y^{2}}}=-1.} lim(x,0)→(0,0)x2−y2x2+y2=lim(x,0)→(0,0)x2−(0)2x2+(0)2=1.{\displaystyle \lim _{(x,0)\to (0,0)}{\frac {x^{2}-y^{2}}{x^{2}+y^{2}}}=\lim _{(x,0)\to (0,0)}{\frac {x^{2}-(0)^{2}}{x^{2}+(0)^{2}}}=1.} Since the two limits are different, the limit DNE. , Multivariable limits are often easier when done in polar coordinates.
In this case, x=rcosθ{\displaystyle x=r\cos \theta } and y=rsinθ.{\displaystyle y=r\sin \theta .} Let’s see how this works. , lim(x,y)→(0,0)xy2x2+y2{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {xy^{2}}{x^{2}+y^{2}}}} , limr→0r3cosθsin2θr2=limr→0(rcosθsin2θ){\displaystyle \lim _{r\to 0}{\frac {r^{3}\cos \theta \sin ^{2}\theta }{r^{2}}}=\lim _{r\to 0}(r\cos \theta \sin ^{2}\theta )} , Although the limit is taken as r→0,{\displaystyle r\to 0,} the limit depends on θ{\displaystyle \theta } as well.
One might then naively conclude that the limit DNE.
However, the limit does depend on r,{\displaystyle r,} so the limit may or may not exist.
Since |sinθ|≤1{\displaystyle |\sin \theta |\leq 1} and |cosθ|≤1,|cosθsin2θ|≤1{\displaystyle |\cos \theta |\leq 1,|\cos \theta \sin ^{2}\theta |\leq 1} as well.
Then |rcosθsin2θ|≤r.{\displaystyle |r\cos \theta \sin ^{2}\theta |\leq r.} , Since limr→0(−r)=limr→0(r)=0,{\displaystyle \lim _{r\to 0}(-r)=\lim _{r\to 0}(r)=0,} by the Squeeze Theorem, limr→0(rcosθsin2θ)=0.{\displaystyle \lim _{r\to 0}(r\cos \theta \sin ^{2}\theta )=0.} Because of the r{\displaystyle r} dependency and the use of the Squeeze Theorem, the quantity in the above limit is said to be bounded.
In other words, as r→0,{\displaystyle r\to 0,} the range of values of rcosθsin2θ{\displaystyle r\cos \theta \sin ^{2}\theta } shrinks to 0 as well, even though θ{\displaystyle \theta } is arbitrary. , lim(x,y)→(0,0)xyx2+y2{\displaystyle \lim _{(x,y)\to (0,0)}{\frac {xy}{x^{2}+y^{2}}}} This example is only slightly different from the one in Example
1. , limr→0r2cosθsin2θr2=limr→0(cosθsin2θ){\displaystyle \lim _{r\to 0}{\frac {r^{2}\cos \theta \sin ^{2}\theta }{r^{2}}}=\lim _{r\to 0}(\cos \theta \sin ^{2}\theta )} However, the quantity cosθsin2θ{\displaystyle \cos \theta \sin ^{2}\theta } can take on an arbitrary value after the limit is evaluated, and is said to be unbounded.
Therefore, the limit DNE.
This scenario is describing a limit being approached from arbitrary directions and getting different values.
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Robert Allen
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